Heterojunction emitter transistor with saturation drift velocity gradient in base

Claim 2

A thermionic emission transistor comprising: an emitter region formed with a semiconductor material having a first conductivity type and a high impurity concentration; a collector region formed with a semiconductor material having the first conductivity type and a high impurity concentration; a base region made of a semiconductor material having a second conductivity type opposite to said first conductivity type and a high impurity concentration, said base region having an impurity concentration distribution such that said base region impurity concentration is maximum in portions adjacent to said emitter region and decreases with distance from said emitter region; and a built-in impurity concentration gradient to generate an electric field of a sufficient magnitude to establish carrier travel velocity in substantially all of said base region at a saturation velocity; that portion of said emitter region located adjacent to said base region having an energy band gap broader than that of the base region and an impurity concentration higher than that of the base region, that portion of said base region located adjacent to the emitter region having an impurity concentration of at least about 3×10 18 cm -3 ; the impurity concentration of said emitter region and the impurity concentration of that portion of said base region located on the emitter region side being set to insure that the width of the depletion layer growing across the pn junction of the emitter and base regions is substantially the same as the mean free path of carriers.

Claim 3

A thermionic emission transistor according to claim 1, wherein the energy band gap of the emitter region is broader by at least 0.1 eV than that of the base region.

Claim 4

A thermionic emission transistor according to claim 1 or 2, wherein there is provided, between said base region and said collector region, a semiconductor region having an impurity concentration lower than that of the base and collector regions and having a conductivity type same as that of the collector region.

Claim 5

A thermionic emission transistor according to claim 1 or 2, wherein the energy band gap of the collector region is broader than that of the base region.

Claim 6

A thermionic emission transistor according to claim 1 or 2, wherein the energy band gap of the collector region is broader by at least 0.1 eV than that of the base region.

Claim 7

A thermionic emission transistor according to claim 1 or 2, wherein the impurity concentration of that portion of the base region located adjacent to the emitter region is about 1×10 19 cm -3 or more.

Claim 8

A thermionic emission transistor according to claim 1 or 2, wherein the impurity concentration of that portion of the base region located adjacent to the emitter region is about 3×10 19 cm -3 or more.

Claim 9

A thermionic emission transistor according to claim 1 or 2, wherein: said collector region at least contains a portion buried in a semiconductor substrate having a conductivity type opposite to that of the collector region and a low impurity concentration, and wherein: said emitter region, said base region and said collector region are provided in a same surface of said semiconductor substrate.

Claim 10

A thermionic emission transistor according to claim 2, wherein the ratio between the impurity concentrations in those end portions of said base region contacting a depletion layer is set at three or greater.

Claim 11

A thermionic emission transistor according to claim 3, wherein the energy band gap of the collector region is broader than that of the base region.

Claim 12

A thermionic emission transistor according to claim 3, wherein the energy band gap of the collector region is broader by at least 0.1 eV than that of the base region.

Claim 13

A thermionic emission transistor according to claim 4, wherein the energy band gap of the collector region is broader by at least 0.1 eV than that of the base region.

Claim 14

A thermionic emission transistor according to claim 3, wherein the impurity concentration of that portion of the base region located adjacent to the emitter region is about 1×10 19 cm -3 or more.

Claim 15

A thermionic emission transistor according to claim 4, wherein the impurity concentration of that portion of the base region located adjacent to the emitter region is about 1×10 19 cm -3 or more.

Claim 16

A thermionic emission transistor according to claim 3, wherein the impurity concentration of that portion of the base region located adjacent to the emitter region is about 3×10 19 cm -3 or more.

Claim 17

A thermionic emission transistor according to claim 4, wherein the impurity concentration of that portion of the base region located adjacent to the emitter region is about 3×10 19 cm -3 or more.

Claim 18

A thermionic emission transistor according to claim 3, wherein said collector region at least contains a portion buried in a semiconductor substrate having a conductivity type opposite to that of the collector region, and wherein said emitter region, said base region and said collector region are provided in a same surface of said semiconductor substrate.

Claim 19

A thermionic emission transistor according to claim 4, wherein said collector region at least contains a portion buried in a semiconductor substrate having a conductivity type opposite to that of the collector region, and wherein said emitter region, said base region and said collector region are provided in a same surface of said semiconductor substrate.

Claim 20

A thermionic emission transistor according to claim 6, wherein said collector region at least contains a portion buried in a semiconductor substrate having a conductivity type opposite to that of the collector region, and wherein said emitter region, said base region and said collector region are provided in a same surface of said semiconductor substrate.

Claim 21

In a transistor of the type including emitter, base and collector semiconductor regions, relatively disposed to provide a controllable current path for carriers emitted from said emitter region through said base region to said collector region, the improvement wherein: said emitter region is formed of a semiconductor material of a first conductivity type, having a first energy band gap, and having a high impurity concentration; said base region is formed of a semiconductor material having a second energy band gap less than said first energy band gap and of a second conductivity type opposite to said first conductivity type disposed adjacent to said emitter region and forming a hetero-junction therewith, said base region having an impurity concentration distribution such that said base region impurity concentration is maximum in portions adjacent to said hetero-junction and decreases with distance from said hetero-junction; and a built-in impurity concentration gradient to generate an electric field of a sufficient magnitude to establish carrier travel velocity in substantially all of said base region at a saturation velocity; said base having a predetermined impurity distribution concentration, the impurity concentration of said base region being at least 3×10 18 cm -3 in portions adjacent to said hetero-junction; and said transistor further includes a built-in depletion layer extending from said hetero-junction having a width no more than the mean free path of carriers in said base region, such that carriers are emitted from said emitter region due to thermal motion travel through said depletion layer without scattering directly into said base region, whereby a high current density is provided.

Claim 22

In a transistor of the type including emitter, base and collector semiconductor regions, relatively disposed to provide a controllable current path for carriers emitted from said emitter region through said base region to said collector region, the improvement wherein: said emitter region is formed of a semiconductor material of a first conductivity type, having a first energy band gap, and having a high impurity concentration; said base region is formed of a semiconductor material having a second energy band gap less than said first energy band gap and of a second conductivity type opposite to said first conductivity type disposed adjacent to said emitter region and forming a hetero-junction therewith, said base region having an impurity concentration distribution such that said base region impurity concentration is maximum in portions adjacent to said hetero-junction and decreases with distance from said hetero-junction; and a built-in impurity concentration gradient to generate an electric field of a sufficient magnitude to establish carrier travel velocity in substantially all of said base region at a saturation velocity; said base having a predetermined impurity distribution concentration, the impurity concentration of said base region being at least 3×10 18 cm -3 in portions adjacent to said hetero-junction; and said transistor further includes a built-in depletion layer extending from said hetero-junction having a width no more than the mean free path of carriers in said base region, such that carriers are emitted from said emitter region due to thermal motion travel through said depletion layer without scattering directly into said base region, whereby a high current density is provided.